INTERNATIONAL CONFERENCE GIREP EPEC 2015 July 6-10, Wrocław, Poland
THE JUBILEE OF THE 70TH ANNIVERSARY OF THE POLISH ACADEMIC COMMUNITY Page | 1 IN WROCŁAW
Europhysics Conference The Conference of International Research Group on Physics Teaching (GIREP) European Physical Society - Physics Education Division (EPS PED), University of Wrocław (UWr)
Key Competences in Physics Teaching and Learning
Proceedings
Wrocław 2016
Page | 2
Published by
Institute of Experimental Physics
University of Wrocław
Pl. M. Borna 9, 50-204 Wrocław, Poland
ISBN: 978-83-913497-1-7
INTERNATIONAL CONFERENCE GIREP EPEC 2015 July 6-10, Wrocław, Poland
Page | 3 THE JUBILEE OF THE 70TH ANNIVERSARY OF THE POLISH ACADEMIC COMMUNITY IN WROCŁAW
Europhysics Conference The Conference of International Research Group on Physics Teaching (GIREP) European Physical Society - Physics Education Division (EPS PED), University of Wrocław (UWr)
Key Competences in Physics Teaching and Learning
Proceedings
Editors
Ewa Dębowska, Tomasz Greczyło
Wrocław 2016
Committees
Honorary patronage Polish Physical Society, Warsaw, Poland Prof. dr. hab. Marek Bojarski, Rector of University of Wrocław, Poland Cezary Przybylski, Marshal of Lower Silesia Voivodeship, Poland Page | 4 Scientific Advisory Committee Mojca Čepič, EPS-PED Committee, University of Ljubljana, Slovenia Costas Constantinou, EPS-PED Committee, University of Cyprus, Cyprus Ewa Dębowska, Chair of the Organizing Committee, University of Wroclaw, Poland Leoš Dvořák, GIREP and ICPE Committee member, Charles University in Prague, Czech Republic Ton Ellermejer, MPTL Committee member, CMA , Amsterdam, The Netherlands Francisco Esquembre, MPTL Committee member, University of Murcia, Spain Hendrik Ferdinande, EPS-PED Committee member, retired at University of Gent, Belgium Raimund Girwidz, MPTL President, Universiy of Ludwigsburg, Germany Zofia Gołąb-Mayer, Jagiellonian University, Cracow, Poland Claudia Haagen- Schuetzenhoefer, GIREP Vicepresident, University of Graz, Austria Zdeňka Koupilová, EPS-PED Committee member, Charles University in Prague, Czech Republic Robert Lambourne, ICPE Committee member, The Open University, United Kingdom Ian Lawrence, GIREP past-Vicepresident, Institute of Physics, United Kingdom Marisa Michelini, GIREP President, University of Udine, Italy Cesar Eduardo Mora Ley, LAPEN President, National Polytechnic Institute, Mexico Andreas Mueller, University of Geneva, Switzerland Hodeo Nitta, ICPE President, Tokyo Gakugei University, Japan Wim Peeters, GIREP Vice-president, DKO (vzw) and PONTon vzw, Belgium Gorazd Planinšič, EPS-PED past Chair, University of Ljubljana, Slovenia Julias Salinas, IACPE and CIAREF President, Argentina David Sands, EPS-PED Chair, University of Hull, United Kingdom Dagmara Sokołowska, GIREP General Secretary, Jagiellonian University, Cracow, Poland Fatih Taşar, iSER President, Gazi University, Turkey Urbaan Titulaer, EPS-PED Committee member, retired at University of Linz, Austria Laurence Viennot, EPS-PED Committee member, retired at University Denis Diderot Paris 7, France Nicola Vittorio, EPS-PED Committee member, University of Rome, Italy Stamatis Vokos, APS T-TEP Chair, University of Seattle, USA Els de Wolf, University of Amsterdam, the Netherlands Dean Zollmann, AAPT representative, Kansas State University, USA
Local Organizing Committee Małgorzata Bacia, Director of Lower Silesian Centre for Teacher Training, Wrocław, Poland Ewa Dębowska, Chair of the Organizing Committee, University of Wrocław, Poland Tomasz Greczyło, Chair of the Local Organizing Committee, University of Wrocław, Poland Bernard Jancewicz, Chair of Wrocław Division of Polish Physical Society Jerzy Jarosz, University of Silesia, Katowice, Poland Elżbieta Kawecka, Computer Assisted Education and Information Technology Centre, Warsaw, Poland Wojciech Małecki, Director of the Regional Examination Board in Wroclaw, Poland Piotr Skurski, University of Lodz, Poland Dagmara Sokołowska, Jagiellonian University, Cracow, Poland Bartosz Strzelczyk, University of Wrocław, Poland
Contents Editors’ Preface ...... 8 Part I ...... 9 Towards Key Competences ...... Page | 5 Learning Physics Using Modern Efficient Methods ...... 10 Lorena Kelo ...... You Haven’t Seen Radioactivity Yet? ...... 17 Vladimír Vícha, Jan Koupil, Jitka Svobodová ...... A Teaching Proposal: Mechanical Analog of an Over-Damped Josephson Junction ...... 25 Roberto De Luca, Immacolata D’Acunto, Roberto Capone ...... Teachers´ Competencies in the Use of Digital Technologies to Support Inquiry in Classroom ...... 30 Zuzana Ješková, Trinh-Ba Tran, Marián Kireš, Ton Ellermeijer ...... Physical - Mathematical Modelling in Physics Teaching ...... 38 Gesche Pospiech, Marie-Annette Geyer ...... Assessment of STEM-design Challenges: Review and Design ...... 45 Leen Goovaerts, Mieke De Cock, Wim Dehaene...... Enquiry for Physics Teachers Following the TEMI Methodology ...... 52 Sara Barbieri, Marina Carpineti, Marco Giliberti ...... Professionalization through Practical Training. The Application of Pedagogical Content Knowledge within the Physics Teaching-Learning-Lab ...... 58 Susan Fried, Thomas Trefzger ...... Analysis of Problem Solving Processes in Physics Based on Eye-Movement Data ...... 64 Eizo Ohno, Atsushi Shimojo, Michiru Iwata ...... Using a Cognitive Hierarchy to Evaluate Physics Problems and to Reform Physics Curriculum . 71 Raluca Teodorescu , Gerald Feldman ...... Physics Teaching and Learning Reform in Armenian Schools: An Impact Study ...... 79 Julietta Mirzoyan ...... Seemingly Unique Devices – How to Use “Nonsenses” in Physics Teaching ...... 86 Vera Koudelkova ...... Improving of Students’ DIY Skills by an Example of Key Competences Development at Science Centres in Ukraine ...... 90 Nataliya Kazachkova , Iryna Salnyk , Pavlo Mykytenko ...... How Worksheets Based on Data from Astronomical Catalogues Influence Key Competences ...... 98 Ota Kéhar ...... Teacher Participants in the European Project TEMI Practice the Enquiry Methodology in Their Classroom ...... 102 Sara Barbieri, Marina Carpineti, Marco Giliberti ...... Summary and Typology of Astronomy Popularization in the Czech Republic ...... 109 Radek Kříček ......
Part II ...... 116 Educational Development and Research ...... The Preservice Teachers’ Conceptions after Training about Ionic and Electron Conduction in Simple Electric Circuit: An Exploratory Study ...... 117 Abdeljalil Métioui, Louis Trudel ...... Page | 6 Assessing the Professional Vision of Preservice Teachers in the Teaching-Learning-Lab Seminar ...... 123 Florian Treisch, Susan Fried, Thomas Trefzger ...... Teachers` Inquiry and Assessment Skills Developed within In-Service Teacher Training Course 130 Marián Kireš, Zuzana Ješková ...... The Position of Experiments in Grammar School Students’ Semantic Space ...... 138 Petr Kácovský ...... Teaching Physics to Non Physicist: Physics for Agricultural, Biotech and Environmental Sciences ...... 142 Marisa Michelini, Alberto Stefanel ...... Implementation of Discussion Method to Favour Physics Problem Solving among High School Students ...... 150 Louis Trudel , Abdeljalil Métioui ...... Theoretically and Empirically Based Evaluation of Laboratory Courses – PraQ Questionnaire .... 156 Daniel Rehfeldt , Volkhard Nordmeier ...... Galilean Relativity Conceptual Understanding versus Subjective Interpretation in Kinematics’ Problems: Cartesian Graphs and Questions ...... 163 Marina Castells ...... Testing the Effectiveness of Drama-Oriented Teaching Methods in a Physics Classroom ...... 173 Arne Traun , Claudia Haagen-Schützenhöfer ...... Part III ...... 180 Teaching-Learning Practices and Classroom Ideas ...... Teaching Energy in the Light of the History and Epistemology of the Concept ...... 181 Manuel Bächtold, Valérie Munier, Muriel Guedj, Alain Lerouge, André Ranquet ...... Enquiring the Higgs Mechanism: A Path for Teachers ...... 188 Sara Barbieri, Marco Giliberti ...... Helping Students Explore Concepts Relating to the Electric Field at Upper Level Secondary Science Education ...... 195 Richard Moynihan, Paul van Kampen, Odilla Finlayson, Eilish McLoughlin...... Integration of some general topics into the introductory physics course for non-physicists – a good practice? ...... 202 Tomaž Kranjc, Nada Razpet ...... Space Science in Thermodynamics ...... 207 Annamária Komáromi ...... General Relativity for Secondary School Students ...... 212 Matěj Ryston ......
Bottle-and-Water-Jet Demonstration of Free-Fall Weightlessness: Do High School Students Know it and what are Their Explanations? ...... 218 Jasmina Baluković, Josip Sliško ...... Problems With Physics-Related Contexts in Mathematics Textbooks for Mexican Secondary School: Some Alarming Examples of Artificial Problem Contextualizations ...... 225 Page | 7 Josip Sliško, Adrián Corona Cruz, Honorina Ruiz Estrada, Rosario Pastrana-Sánchez ...... A Sequence to Teach Quantum Mechanics in High School ...... 234 Sergej Faletič ...... Terrain Experiments With Datalogger in Physics Teaching in Higher Secondary Education ...... 242 Peter Demkanin, Jozef Trenčan ...... The Effects of Different Phases of a Predict-Observe-Explain Activity on Students’ Learning about Buoyancy ...... 250 Jelena Radovanović, Josip Sliško, Ivana Stepanović Ilić ...... An Inquiry-Based Approach to the Learning of Dynamic Equilibrium by Means of the Argentine Tango ...... 256 Nicola Pizzolato, Dominique Persano Adorno...... Irregular Chaos in a Bowl ...... 262 Péter Nagy, Péter Tasnádi ...... From Galileo’s Clepsydra to Webcamera: Methods of Tracing of Motion in Teaching Physics ... 270 Zsanett Finta ...... Strategies of Students to Solve Physics Problems with Unreasonable Results ...... 275 Alejandro González y Hernández, Josip Sliško ...... Examples of Best Practice for Cross-Age Peer Tutoring in Physics ...... 283 Marianne Korner, Martin Hopf ...... Collection of Solved Problems in Physicc: Online Learning Source Encourages Students' Active Learning ...... 288 Zdeňka Koupilová, Dana Mandíková, Marie Snětinová, Krzysztof Rochowicz, Grzegorz Karwasz ...... How to Increase Teachers’ Self-Confidence: An Example Concerning Semiconductors...... 292 Leoš Dvořák ...... Comparing Traditional Pedagogical Approches in Science to Inquiry Based Ones: A Case Study with Pre-Service Primary School Teachers ...... 298 Giuliana Croce, Onofrio R. Battaglia, Claudio Fazio ...... Teaching Biophysics at the Faculty of Rehabilitation, Józef Piłsudski University of Physical Education in Warsaw ...... 304 Michał Wychowański, Janusz Jaszczuk, Barbara Łysoń, Andrzej Wit ...... Authors index ...... 310
Editors’ Preface
The volume presents the Proceedings of the GIREP EPEC 2015 Wrocław International Conference consisting of the papers submitted by the participants of the event.
Page | 8 We have tried to do our best to group authors’ proposals thematically following both,
domains:
I. Researching formation of Key Competences in physics teaching and learning – new research approaches, new methods, innovative learning strategies, new models; II. Key Competences changing pedagogy – formative assessment, teacher role, student role, KC oriented assessment, shared pedagogy, KC oriented pedagogy; III. Developing of Key Competences – examples of good practices;
and groups:
A. Research (physics education research, empirical as well as theoretical levels); B. Research and development (including classroom ideas, practical issues, development etc. being more substantial than research); C. Classroom ideas, teaching and learning practice (no or minimal research part).
As a result of the grouping process three chapters were created: Towards Key Competences, Educational Development and Research, Teaching-Learning Practices and Classroom Ideas.
The Organizing Committee received a large number of proposals and selection involved very careful decisions. Due to diversity of proposals and richness of the subjects suggested by the authors it appeared to be not an easy task and resulted in preparation of two publications. The one entitled “Key Competences in Physics Teaching and Learning” and containing selected contributions was published by Springer, and the second one, Proceedings of the Conference, you are reading now. We hope that the authors, the participants of the event and the readers will be satisfied by the organization and content of each volume.
The conference language – English – is rich, complex and dynamic. Considering that for most people English is not their mother tongue, it is little wonder that the structures and nuances vary significantly across nations. The Proceedings are the output of the international conference; one of their strengths is the ability to be truly representative and inclusive. That is why we prefer the essence of the matter on its style and content and the way it is presented. As a result one can find in the volume phrases or sentences that might not fit with some rules of English grammar, for what we do apologize, but we are proud that during the review process no work was rejected because of deficiencies in its use of language.
Each paper was reviewed by at least two reviewers. The organizers are grateful to the authors for their enthusiasm and to all the reviewers for their painstaking work and the time they devoted to the evaluation process.
Ewa Dębowska and Tomasz Greczyło
Editors
Page | 9
Part I
Towards Key Competences
Learning Physics Using Modern Efficient Methods
Lorena Kelo Faculty of Natural and Human Science. University of Korce, Albania
Abstract Page | 10 After a research on teaching Physics in the world and the achievements of the last decades in this field, this article treats an approach based on the experiences of the Department of Physics and Information of the University of Korce. As part of this Faculty I felt it necessary to review the classical methods of teaching physics in our faculty, where the teacher’s role is mainly descriptive, dominant, and not collaborative. We tried to apply the interactive method of teaching physics where the teacher’s role is mainly consultative and/or advisory. Comparison of the results of the two methods indicate the primacy of interactive method. Nowadays, the Theory of Cognitive Processes, in progress, and the Teaching of Physics, are based on well- defined scientific regulations and laws. The reality presents the need for studies, reconsidering the methods of teaching, through tracing and applying new models, aiming the final goal, the Expertise. Besides, other methods, the methods of interactive work in group improve the efficiency in teaching much more than the methods of explanation, narration, school lecture, instruction, etc., already known as parts of classical methods. So, the main instruction of contemporary didactics is focused on the solution of problems in Physics. Complex problems, term papers and/or tests, serve as yhe means for the estimation of conceptual learning, so that the students’ concepts become practical and useful. Scientifically, the methods of solving complex problems are based on well-known experimented strategies. After the theoretical treatment at the end of this article, you will see the surprising results we obtained, after applying the methods of interactive teaching.
Keywords Cognition, collaborative work, monitoring of knowledge, group learning, complex problems, strategy/solution scheme.
Five principles that should be applied while teaching Physics to the students
With the increase of understanding how the students should study, the teacher has a greater possibility to improve his/her teaching process. Continuous research has shown that Physics has become a discipline that can be taught by using consolidated scientific methods. (Edward F. Redish (2003)) . After a massiveness of didactic research, a set of principles, which the teacher should consider as s/he teaches Physics, has become possible. Here they are: First principle: Teach the students to build conceptual knowledge: This principle suggests that the methods of teaching should give the students the ability to structure new and old knowledge around the main concepts. Second principle: Teach the students to use their previous knowledge. This principle suggests that students should be taught how to use their previous knowledge while acquiring new knowledge. Fourth principle: Teaching should be fit for each student bearing in mind differences among them. Teaching methods should be suitable with the abilities of students with regards to their previous knowledge. Fifth principle: Teaching by doing. Teachers of Physics should engage students in a variety of practices to be used in different situations. (Brown J.S, Collins, A. and Duguid, P (1990)).
Expert of Physics versus Student of Physics
The hierarchic classification of the objectives to be reached by the teacher, so that s/he enables the students to study Physics properly, is given by Bloom’s Taxonomy. In 2001 Marzano improved the Taxonomy by bringing the student from the era of knowledge to that of concepts. In the Revised Taxonomy, the gerunds are substitutes for names of Bloom’s Taxonomy with regards to the successive phases in students’ upbringing; on top of it stands the phase of “creation”. This means that the Revised Taxonomy involves the principle of “Teaching by Doing”; so the final result in contemporary education brings creative abilities. (Morzano, R.J.&Kendall, J.S.(2007)). Figure 1 shows the pyramid of classification of objectives after Bloom (on the left) and after Morzano (on the right). To reach the proper objectives, the teacher indispensably needs to apply contemporary methods. Why it is such indispensable?
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Figure 1. a) Bloom’s Original Taxonomy b) Revised Taxonomy
Contemporary methods of Teaching Physics are interactive and cooperative, whereas classical ones refer to the student as an individual. Indeed these methods differ from each other qualitatively. They are symbolized explicitly by the two figures below (Figure 2). (Smith, K.A.(2010))
(a) (b) Figure 2. Classic teaching (a) versus Interactive teaching (b)
Under the conditions of classical teaching, let’s consider what the students do and what they do not. They focus on defining the answer, but do not analyse the situation in terms of concepts. They build an abstract image about the problem, mainly based on superficial data of the situation, but do not interpret mathematical formalisms. They use a limited way of concepts, but do not try to find alternative solutions. They define the way to solving a problem, mainly involving equations, but do not formulate schemes and/or strategies before solving it. They try to solve the problem using the Physics they already know, but do not compare the problem with similar situations, reflecting personally while solving it. Thus, the main difference between the expert of Physics and the student of Physics lies both in the “way of operating” and in the “structure of knowledge”. It is more important to gain useful knowledge than focus on the amount of knowledge. (Zajchowsk, R. &Martin, J. (1993)) The scholars have shown several special aspects as regards the difference between the expert of Physics and the student of Physics. (M. Dede, F. Vila (1991)). See the table below:
Table 1. Special aspects that shows differences between the expert of Physics and the student of Physics
Steps Student of Physics Expert of Physics Reasons from.... Laws Models Acts with..... Symbols Concrete Situations Solves Defined Problems Real and complex Problems Generates Physical concepts Structured, negotiable and visionary knowledge Knowledge Type..... Discrete Complicated Structure.... Chronological Hierarchic Presentation.... Few, few ideas Lots, lots of ideas Memory..... Short-term Long-term
One of the main objectives why applying contemporary methods is to create experts of Physics not merely students of Physics. Thus, the tasks and estimations (homework, tests and exams) should be keen to encourage creativity to the students of Physics. (Morzano, R.J.&Kendall, J.S.(2007)).
Work in group and the solution of complex problems Page | 12 There are seven basic principles that serve for the organization of interactive and/or cooperative work in group. They are fairly efficient for the education of students (Arthur W. Chickering and Zelda F.Gamson (1987)), aiming the preparation of students as experts of Physics: Encourage the students to contact each other, including the students of other fields of study. Develop reciprocity and cooperation among students and teachers. Use teaching techniques actively. Stimulate quick reaction. Give students enough time to do their homework and/or turn the papers in time. Discuss requirements in a clear communication. Pay special attention to talented students and the ways you teach them. The students are organized in informal groups (short-term, while in classroom), formal groups (long-term, having defined assignments) as well as study groups (Smith K.A, S. F. Schmoberg (1986)). Let us consider how both informal and formal groups are organized. Work in groups includes a long list of aspects which shall be considered below from organization to estimation of efficiency. To solve problems in Physics, we use sets of laws and regulations. So we determine the strategy for a logical solution. This strategy is associated with a tactic, which consequently leads to a practical scheme for solution (M. Dede, F.Vila, (1989)). The duty of the teacher is to fully inform the students about the scheme and ask them to apply it while exercising. The scheme for solution is given in details below: Introduction of problem - Cognition of problem. - Designation of the field/s of Physics where the problem is mixed in. - Physical description of phenomena. - What is known, what is required. - Illustration in diagrams and figures. - Highlight the explicit and/or implicit conditions/ hypothesis. Solving the problem First phase: physical aspect; - Requirements. - Suppositions, referred to explicit and implicit conditions. - Parameters/variables already known. - Equation, which obviously contains the required parameter. - Successive equations, with intermediate unknown data shown in previous equations (we stop writing them in case there are no more unknown intermediate data). - Verification of the total number of written equations, which should be n+1, where the n is the number of intermediate variables. Second phase: Mathematical aspect; - Perform mathematical actions, which lead to a solution with symbols. - Verification of results with the evidence of units (an indispensable condition). Comment of theoretical result; - Discussions for a new and deep physical interpretation. - Discussions of special matters. Comment of quantitative results after the numeric replacement of variables; - Solution with symbols is a substitute for Numeric data. - Discussion of numeric value. Let us consider complex problems, for they are the main element of conceptual learning (Styer, D. (2002)). They include a variety of issues, interlinked with each other, not only in one branch of Physics but also in several branches en bloc.
Organization and estimation of the efficiency of working in groups. Results
To be efficient in solving problems of Physics, the working groups should follow a scientific procedure: that is, a model procedure organized within the groups (Schwaz, Roger. (1994)). There are many versions for such a procedure, however, in essence all versions are organized in accordance with a unique scheme explained below: Clear definition of the problem. A good definition of the problem in Physics clarifies the actual Page | 13 situation and sets the goal to be reached; in other words it facilitates solution. Identification and definition of main links. Links to solving the problem should be organized according to a scheme of “fish type-skeleton/rib”. Each rib is a possible link to solving the problem. Ribs rest on a main line that ensembles them all. This process leads to the final solution. Generation of alternative solutions. After identifying and defining the main links, the group gives spontaneous ideas for an alternative solution, knowing that they shall not be estimated in doing so. By generating alternative solutions, we make possible the integration of better ideas (Tagliere, Daniel. (1993)). Let us focus on practical aspects of teaching in groups, realized with the students of the first course of the branch of Information Technology of the Faculty of Natural Sciences and Humanities of the University of Korce. The students were divided in two groups, A and B. In Group A, we applied the classical method of teaching – the teacher’s role was mainly descriptive; whereas, in Group B, we applied the method of interactive and cooperative teaching – the teacher’s role was consultative and/or advising. During the first semester Group A wrote two intermediate tests, and the students were estimated in points (below, you will see their results compared with those of Group B.) With regards to the procedure we applied in Group B, we are giving the details below:
- Before an exercise class, the teacher spends 5 to 7 minutes, posing a problematic question to the students (usually one that needs multiple answers). With this question, the teacher encourages the students towards a conceptual education. The question is mainly based on parts of a lecture explained beforehand. - The students have the possibility to contribute individually, giving their own answers, while the teacher checks them, and orients students towards the correct answer with the help of additional ancillary questions. - Then the students discuss the question with their ‘neighbors’ in classroom, while the teacher still checks their answers. - The question gets a final answer, after the students discuss and clarify the question. (Beatty, Ian D. & Gerace, William J. altr. (2006)) - Only then, the teacher continues with the solution of problems, strictly following the detailed scheme shown in paragraph 3. The teacher requires that the students also follow that scheme rigorously, while solving problems themselves. Then the students are instantly divided into informal groups and are encouraged to solve a given problem. During the solution, the teacher keeps notes estimating the group as a whole as well as each of the members individually. At the end of the semester, the estimation for each of the students is converted into points (10 points maximum) Another aspect of working in group. The students are organized in formal groups and they are given a defined task. The task includes a theoretical theme of the course of Physics, which they study, complete, and explain, as if they were the teacher. They are estimated with points, for every aspect of their performance (10 points maximum). The formal groups are also given a complex problem. They should solve the problem following the scheme that the teacher has applied while in the session of solving problems (M. Dede, F. Vila (1991)). After solving the problem, members of each group are estimated with points (10 points maximum). At the end of the semester the students take the final examination. The amount of points obtained during the semester is added to the points obtained in the final examination. These points are then converted into the final grade for the semester. The abovementioned results are summarized in the table below:
Table 2. Interim results for the students of Group B, and their final results.
High Theme Complex Activation Total Final school in problems while in points of exam Student average group in group class, interim (max Grade* grade points points homework results 70 (max (max 10 in points (max 30 points) Page | 14 10 points) (max 10 points) points) points) Student 1 8.8 10 7 10 27 50 8 Student 2 5.6 3 5 4 12 19 4 Student 3 9.2 9 6 10 25 41 7 Student 4 7.17 3 4 6 13 31 5 Student 5 6.7 7 4 3 14 28 5 Student 6 5.32 5 4 3 12 15 4 Student 7 9.37 8 4 7 19 54 8 Student 8 7.47 8 8 4 20 32 6 Student 9 5.65 2 2 4 8 20 4 Stud. 10 6.6 5 5 4 14 28 5 Stud. 11 9.57 10 6 10 26 47 8 Stud. 12 8.29 5 5 10 20 32 6 Stud.13 6.98 4 5 4 23 31 6 Stud. 14 7.05 4 6 5 15 46 7 Stud.15 7.25 0 0 3 3 15 4 Stud. 16 6.72 5 3 5 13 29 5 Stud. 17 5.6 2 0 1 3 18 4 Stud. 18 7.32 8 4 4 16 37 6 Stud. 19 5.72 5 5 6 16 26 5 Stud. 20 6.95 6 5 4 15 28 5
We have coloured table 2 to distinguish formal groups from Points (Final exam + Grade each other. * Based on the regulations of the University of interim results) Korce, the students can obtain a maximum of 30 points 0 - 39 Non-passing grade 4 during the semseter (these are called interim result points) 40 - 50 5 Conversion of these points into grades is shown. 51 - 60... 6... Below are the results for the Group A: 91 - 100 10
Table 3. Interim results for the students of Group A, and their final results.
High school First Partial Second Activation Total points Final average Test Partial Test while in class, of interim Exam Student grade In points In points homework in results (max 70 Grade (max 10 (max 10 points (max 10 (max 30 points) points) points) points) points) Student 1 5.9 2 3 3 8 15 4 Student 2 7.64 4 6 9 19 24 5 Student 3 5.7 3 3 5 11 21 4 Student 4 8.35 6 5 9 20 43 7 Student 5 7.84 5 5 6 16 37 6 Student 6 6.43 4 4 5 13 20 4 Student 7 7.89 4 5 5 14 29 5 Student 8 9.32 8 8 9 25 42 7 Student 9 6.7 5 3 4 12 31 5 Stud. 10 8.57 7 6 9 22 34 6 Stud. 11 6.1 3 4 3 10 17 4 Stud. 12 7.72 6 5 7 18 25 5 Stud. 13 5.9 1 0 2 3 10 4 Stud. 14 9.4 8 9 7 24 51 8 Stud. 15 7.73 7 7 6 20 33 6 Stud. 16 6.64 6 5 5 16 30 5 Stud. 17 7.39 5 7 6 18 35 6 Stud. 18 5.1 4 2 2 8 16 4 Stud. 19 7.8 2 3 5 10 21 4 Stud. 20 6.34 1 3 2 6 15 4
If we carefully examine the results of all the students, we realize that the results of Group B are much higher than those of Group A. The passing rate of students in Group B is 15% higher than that of the students from the Group A. Furthermore, the average grade of the students from the Group B is higher than that of the students from the Group A. With reference to such results, we conclude that the interactive method is more efficient than the classical method. The results analysed in this article are modest but exciting for a faculty like ours. I'm determined to continue applying the methods proposed in this article, and enrich the list of positive results, as a proof to change our classical methods of teaching physics. Applying this method, the stronger students Page | 15 developed their special abilities to a higher level. It also helps weaker students to deepen their concepts in Physics. It develops a great communication among teachers and students, treating the latter as active partners.
Recommendation
Perspectives are changing drastically. The teaching process should be supported by powerful scientific methods which are proven to be successful. Interactive work in groups is the most efficient model in Physics. Based on good results achieved and discussed in this article, the departments in our faculties should be encouraged to use the interactive method in Teaching Physics, because teaching is not only a lecturer property but it's a collaboration work between students and lecturers, and students with each other. Solving problems is the main goal of conceptual teaching. The solution of problems is facilitated through the use of scientific strategies/schemes. Analysing of basic principles that guarantee success and quality in teaching, getting to know what guarantees such principles dealt with in general terms, gave us the chance to present several thoughts on the Methodology of Physics. Choosing this theme as a suggested class model aimed the objective that the knowledge on Physics such as recognition, understanding, application, analysis, generalization in studying occurrences, connection of amounts, discovery of laws, conditions in application, essential principles, etc., has to ensure an active cooperation between the lecturer and the student to follow every step through which scientific knowledge is conveyed in realizing the objectives of scientific research: To discover new facts. To verify and prove important facts. To analyse an occurrence or process in which cause-result relation is identified.
References journal papers Beatty, Ian D. & Gerace, William J. altr. (2006): Designing effective questions for classroom response system teaching. American Journal of Physics, 74(1), p. 31-39 Brown J.S, Collins, A. and Duguid, P. (1990): Situated cognition and the culture of learning. Educational Researcher, 18(1), p. 32-41 Styer, D. (2002): Solving Problems in Physics, Oberlin College, Ph.Dept http://www.oberlin.edu/physics/dstyer/SolvingProblems.html Zajchowsk, R.&Martin, J.(1993): Differences in the problem solving of stronger and weaker novices in physics: Knowledge, strategies, or knowledge structure? Journal of Research in Science Teaching, 30(5), 459-470. 9th Common Conference of the Cypros Physics Association and Greek Physics Association.
books Arthur W. Chickering and Zelda F.Gamson (1987) Morzano, R.J.&Kendall, J.S.(2007). "The New Taxonomy of Educational Objectives", 2nd Ed. CA: Corwin Press Schwaz, Roger. (1994). "The Skilled Facilitator. Practical Wisdom for Developing Effective Groups". Jossey-Bass Publishers, p.314 Smith K.A "Cooperative learning groups" in S. F. Schmoberg (ed.) Strategies for Active Teaching and Learning in University Classrooms. Minneapolis: Office of Educational Development Programs, University of Minnesota, 1986.
paper in conference proceedings M. Dede, F. Vila (1991): On the conception and logical scheme of the complex physics problem’s solution Proceedings of 1st General Conference of BPU, Thessaloniki, Greece, Vol.1, p. 26-29
papers in books Edward F. Redish (2003). "Teaching Physics with Physic suite", John Wiley & Sons, Vol.1, p.216. Smith, K.A.(2010) "From small groups to learning communities", New Direction for teaching and Learning, 123, p. 11-22 Tagliere, Daniel. (1993). "How to Meet, Think, and Work to Consensus", Pfeiffer & Company p.142
Affiliation and address information Lorena Kelo Faculty of Natural and Humans Science Departament of Mathematics, Physics and Informatics University of Korce Shëtitore "Rilindasit", Korce Albania Page | 16 e-mail: [email protected]
You Haven’t Seen Radioactivity Yet?
Vladimír Vícha, Jan Koupil, Jitka Svobodová Institute of Experimental and Applied Physics (IEAP), Czech Technical University in Prague, Horská 3a/22, CZ 12800 Prague 2, Czech Republic
Page | 17 Abstract Radioactivity and particle physics are parts of physics that are very abstract for pupils, partly because teachers usually cannot perform any experiment from these fields. Because of this, radioactivity is somewhat covered in a cloak of mystery and fear. In our workshop we tried to introduce a new educational device – the particle camera MX-10 – that enables us to see radioactivity and enter the world of elementary particles and relativistic energies. Workshop participants had an opportunity to experience visualization of radioactivity and to measure properties of radiation of a few safe radioactive sources (uranium glass, welding electrode with thorium, potassium sulfate, americium) and of the natural radiation background.
Keywords MX-10, IEAP, radiation, radionuclides, uranium, thorium, potassium, americium, muon.
The particle detection principle of a MX-10 camera
The technology we are using is based on a Medipix family chip. The story of the Medipix chip goes back to 1990s when it was developed by the Medipix collaboration under the supervision of CERN. Since then, the detectors have been tested in many applications and fields, such as radiation monitoring in CERN and in space, in material analysis or medical imaging. The MX-10 camera (fig. 1) is manufactured by a Czech company Jablotron in cooperation with the IEAP and it is a device designed especially for educational purposes.
Silicon sensor
USB cable
Figure 1. Particle camera MX-10
The heart of the camera is a Timepix silicon pixel detector. The chip can detect impacting ionizing particles and measure their deposited energies. The chip is 300 µm thick, 14 by 14 mm wide, and is split into 256 by 256 pixels that operate in a way similar to a digital camera. In such arrangement the device visualizes ionizing particle tracks similarly to a cloud chamber or a photographic emulsion but with the recording and analysis capabilities of a computer. A schematic picture of a Timepix detector can be found in fig. 2. The control software (Pixelman) for the Medipix or later Timepix detectors was developed and licensed by the IEAP in Prague, a simplified version called Simple Preview has been developed for educational purposes.
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Figure 2. A schematic picture of a Timepix detector (MX-10). Figure published in [1].
Visualization of radioactivity and energies of primary radionuclides
The first task is to try detection of primary radionuclides and at the same time to familiarize with the basic controls and possibilities of the Simple Preview software that controls the MX-10 detector, processes and visualizes measured data into particle tracks, ranks them and determines absorbed energies. The nuclei of the primary radionuclides as well as stable isotopes were created by thermonuclear synthesis in interior parts of stars or by nucleogenesis during explosions of supernovas. The nuclei that had a short half-life (compared to the age of Earth), decayed and they no longer occur in the nature. We can come across only those ones that have half-life at least ten to the power of eight years (108 years). The most important primary radionuclides are potassium 40Ca, thorium 232Th, uranium 235U and uranium 238U. At the beginning we are going to study uranium glass radiation. Uranium glass is commonly used in crafting decorative things such as beads or vases and it is a traditional Czech product. Tracks of particles emitted from uranium glass can be differentiated into three categories corresponding to the alpha, beta and gamma radioactivity. Take a bead from uranium glass (fig. 3 left), bring it close to the detector and record one minute of ionizing radiation tracks. We should receive an image similar to fig. 3 right.
Figure 3. Uranium glass (left) and visualization of its radiation (right). Exposure time was 60 s. The snapshot contains 3 alpha particle tracks, 146 beta tracks and 34 gamma tracks.
The snapshot depicts uranium glass radioactivity. We can see that it contains the three basic types of tracks. The software has classified the particles and counted them. Using the magnifier tool we can magnify selected tracks
(fig, 4 and fig. 5) to study their characteristic shapes and determine energy they have deposited inside the sensor. Alpha tracks have a typical shape of a wide round blob and a typical energy is of the order of thousands keV. Beta particle tracks are long and curvy – their shape is often worm-like. Their energies are of the order of tens or hundreds of keV (fig. 4). Gamma photon tracks are usually one pixel events with absorbed energy typically of the order of tens keV. (fig. 5).
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Figure 4. Left: an alpha particle track. Energy deposited inside the detector was 2 409 keV. Right: beta particle track, 661 keV of deposited energy.
Figure 5. Gamma photon track – single pixel sized. Energy absorbed by the detector was 14 keV.
After the first measurement we made one-minute-long measurement using other primary radionuclides: welding rod WTh-40 that contains thorium and potassium sulfate (common weed fertilizer), see fig. 6. Now we can compare all three sources. The radiation of the electrode and uranium glass is similar – containing all three kind of radioactivity, however the welding rod emits alpha particles more often. The potassium emits only beta and gamma radioactivity.
Figure 6. Visualization of radioactivity: thorium 232Th (left) and potassium 40K (right). Exposure was 60 s for both cases.
There are a few observable differences between the radiation sources. Both uranium and thorium emit all kinds of radioactivity because they form decay series and the radioactivity we observe is emitted not only from primary nuclides but also from all daughter products of decay. In case of thorium we observe a greater amount of alpha radioactivity and further study shows that alpha particle energies can exceed 8 MeV and it is not so in the case of uranium. Potassium does not form decay series because it decays either by beta decay to calcium 40 40 0 Page | 20 19 K20 Ca1e ν , or by a K-capture to argon 40 0 40 * 19 K1e 18Ar ν. The MX-10 camera detects only beta and gamma; it is not capable of detecting neutrinos. We have seen that unstable nuclei can be detected using their radioactivity visualization and particle energies analysis.
The world of relativistic speeds
Einstein’s special relativity is a part of high school curriculum in Czech Republic. This theory predicts effects that are observable only at speeds comparable to the speed of light in vacuum. On the other hand, the speeds of objects around us are negligibly small when compared to the value c = 3·108 m·s-1 and therefore special relativity effects cannot be observed and for students the world of relativistic speeds is very strange. Let’s try to answer the question “Is there anything around us that is almost as fast as light?” We will study the energies of alpha and beta particles that have hit the detector and from these energies we will calculate speeds of these particles. The measuring program determines absorbed energy for each particle and this energy corresponds to kinetic energy Ek (displayed in units keV). From Einstein’s formula E = E0 + Ek we can derive for particle velocity: 1 v c 1 . Ek 1 E0 Let us choose a few alpha particle tracks (source: uranium glass, thorium electrode) that have deposited high energies in the detector, and calculate alpha particle speeds.
Table 1. Speeds of alpha particles emitted by uranium and thorium
Ek [keV] 6 824 7 626 8 733 5 990 v [m·s-1] 1.81·107 1.91·107 2,05·107 1.70·107 v/c ·100 % 6.0 6.4 6.8 5.7
Second row of table 1 shows that the speeds of alpha particles are very high, of the magnitude of order 107 m·s-1. Third row contains comparison of alpha particle speed and light speed – we can see that the ratio magnitudes are 1 of the order of units of percent which means that the non-relativistic formula for kinetic energy E mv 2 k 2 should be accurate enough. Now let’s examine some of the higher energies deposited in the detector by beta particles (electrons) emitted by uranium glass, electrode or weed fertilizer. These values are summarized in table 2.
Table 2. Speeds of beta particles
Ek [keV] 384 455 537 625 v [m·s-1] 2.46·108 2.55·108 2.62·108 2.68·108 v/c ·100 % 82.1 84.9 87.3 89.3
The electron speeds (second row of tab. 2) are of the same order of magnitude as the speed of light, their relative speeds exceed 80 % of the speed of light, and moreover we have to take into account that the particles might not have deposited all of their energy in the chip. Their real speeds might have been therefore even higher. It is quite interesting for students that usual potassium flower fertilizer is a source of electrons with relativistic speeds. We can only wonder if people in the gardening centers know that.
Radioactive background on the surface of the Earth
Primary radionuclides are natural radionuclides that form the natural radiation background on Earth (together with cosmic radiation). Using a MX-10 it is possible to monitor the radiation background. Table 3 shows data from 120 seconds long measurements during the workshop. All detectors were oriented vertically. We can see that gamma and beta radioactivity are dominant, alpha is rare. Frame analysis also shows Page | 21 that there are very rare events categorized as “other”. The alpha radioactivity most probably originates from radon or its daughter products, the “other” are usually tracks of muons that are a part of cosmic radiation. Muons are highly penetrating particles, their tracks are not being curved by the material of the silicon chip and therefore they are observed as straight lines (fig. 7). Capturing a muon track is quite rare event since the particle had to be moving within the plane of the detector chip (300 µm thick) or with a very small declination from this plane. A result of such low probability is that a track at least 20 pixels long is captured approximately once in ten minutes.
Figure 7. A long track of a muon (220 pixels)
Table 3. Counts of ionizing particles measured by six independent MX-10 detectors while measuring the radiation background. Time of exposure: 120 s, vertical sensor orientation.
1 2 3 4 5 6 Sum Alpha 0 0 0 1 0 0 1 Beta 14 14 13 12 18 13 84 Gamma 16 15 15 15 17 16 94 Other 0 0 1 0 0 0 1
Visualization of americium radiation and its energies
For demonstrating the basic properties of radioactive radiation it is better to have a safe source that has activity higher than the natural sources described above. Such source might be the ŠZZ ALPHA (241Am, 9.5 kBq, fig. 8 left) that comes as a part of the MX-10 edukit. Americium is a typical source of alpha particles that are also accompanied by gamma photons. The activity of the source is chosen to be categorized as a safe source of radiation (according to Czech national standards), however it is significantly higher than previous sources. During 2 second exposure we have detected over 100 alpha particles (see fig. 8 right).
Figure 8. ŠZZ ALPHA radiation source (241Am, 9.5 kBq) (left). Tracks of alpha and gamma radiation (right). Exposure time: 2 seconds.
For further exploration of americium radiation we have used analytical tools of the Simple Preview program: the energy histogram (fig. 9) and the particle count histogram (fig. 10). The actual value of energy for alpha particles emitted by americium 241 is 5.5 MeV, however our graph has a peak for energy around 3.5 MeV. This is due to energy loss that occurs partly even inside the americium itself, partly inside the thin golden film that covers the americium, and finally during the propagation through air.
Fig. 10 shows that the count of particles in one frame is a random quantity with mean value of 20 particles. The Page | 22 data corresponds very well to Poisson distribution.
Figure 9. Alpha particles energies (americium in the ŠZZ ALPHA).
Figure 10. Histogram of counts of alpha particles detected in one frame
Figure 11. Histogram of alpha radiation energies for source close to the detector (right peak, mean energy 3.5 MeV) and displaced by 1 cm (left peak, mean energy 2.1 MeV).
Absorption of alpha radiation
The energies of alpha particles are significantly higher than energies of beta or gamma, on the other hand alpha radiation has highest ionizing effects and therefore it is the least penetrating. In the air alpha particles with energies around 3.5 MeV can reach 2.1 cm. The next experiment shows how to determine using a histogram how much energy an alpha particle approximately loses while penetrating 1 cm of air. Fig. 11 shows two energy Page | 23 peaks, the first was measured with source placed as close to the detector, as possible, while the second one with the source moved by 1 cm. The difference of mean energy of the peaks is approximately 1.4 MeV and this difference equals to energy that has been lost during the particles’ path through air.
The following two experiments study absorption of alpha radiation in paper and in water. Fig. 12 left shows tracks detected after we placed a sheet of common paper between the chip and the radiation source (only top-left corner of the chip is covered). We can see that while alpha radiation does not penetrate the paper, gamma radiation does. During the next experiment we placed a thin food wrapping stretch film on the detector and placed a small droplet on it (fig. 12 right). We can see a “shade” of the droplet and we can conclude that while alpha particles can penetrate the film, it cannot penetrate water (even a very thin layer). Gamma photons are penetrating both the film and water.
Figure 12. Alpha radiation absorption in paper (left) and in water droplet (right) placed on stretch film. Gamma photons penetrate paper, film and water.
Absorption of gamma radiation
Gamma photons are being differently absorbed by different materials based on atomic number of elements that form these materials. This property of gamma radiation has quickly started being used in medicine and engineering for the so called X-ray imaging.
Let’s show how to make a radiographic image: we placed different metal objects into plastic boxes and workshop participants had a task to discover what is inside without opening/destroying the boxes. They received a “black box”, placed it between the americium source and detector and created an image with long exposure time (several minutes’ exposure – fig. 13 right).
Figure 13. Placement of a black box onto the detector (left). A radiography of steel pad. The image also contains two long muon tracks.
Conclusion
In our workshop we tried to present a set of experiments suitable for direct use in teaching basic properties of radioactivity and ionizing radiation. Because all of the used sources of radiation are safe (in both medical and legal terms), these experiments might be used not only as demonstrations but as student labs as well. A more extensive textbook containing ca. 50 experiments with the MX-10 camera should be available very soon. Page | 24 References [1] Platkevič, M. (2014). Signal Processing and Data Read-Out from Position Sensitive Pixel Detectors, dissertation thesis, Czech Technical University in Prague. [2] Medipix collaboration, the Medipix homepage [Online]. Available at: http://medipix.web.cern.ch/medipix/.
Affiliation and address information Vladimír Vícha, Jan Koupil, Jitka Svobodová Institute of Experimental and Applied Physics Czech Technical University in Prague Horská 3a/22 128 00 Praha 2 Czech Republic e-mail: [email protected], [email protected], [email protected]
A Teaching Proposal: Mechanical Analog of an Over-Damped Josephson Junction
Roberto De Luca, Immacolata D’Acunto, Roberto Capone Department of Physics “E. R. Caianiello”, University of Salerno, Italy
Page | 25 Abstract An over-damped pendulum can be adopted as a mechanical analog of an over-damped Josephson Junction. The basic equations leading to the driving torque versus time average of the angular frequency are studied. The mechanical analog can be used to provide additional insight into the current-voltage characteristics of over- damped Josephson Junctions.
Keywords Teaching , Josephson Junction, Analogy, Physics Education,
A Teaching Proposal
Why should we talk about Josephson Junctions (JJs) to high school students? In Italy the topics of modern Physics are often presented, according to a historical approach, during the last year of scientific High School. An experimental approach is rarely applied. “In order to enter into the quantum mechanics world it is necessary to make a big conceptual leap which can be, for example, the abandonment of the classical idea of "trajectory", to which we are so well accustomed because of our everyday experience” (Rinaudo 2003). We also have to withdraw from which student have become familiar during high school studies. The JJs allow us to refer to many practical applications such as electronic devices, SQUIDs, quantum computers or magnetoencephalography (Barone 1982). The Physics behind these applications can intrigue and motivate students to study more meaningfully. The complexity of the phenomena related to JJs can be overcome through a simple analogy: an overdamped pendulum. Under over-damped conditions, this analogy is summarized in Table 1.
Table 1. Analogy between Josephson Junction and an over-damped pendulum.
Josephson Junction Pendulum
Phase difference Angular position θ
Bias current Applied torque
Capacitance Moment of inertia